Analysis process of a line transfer photosensitive device and operating device of such a process

ABSTRACT

The present invention concerns an analysis process of a line transfer photosensitive device. 
     The charge-signal and the charge noise transfers from the columns towards the memory have the same duration and are made by using a same training charge, stored in memory, that must be at least sufficient to allow to pass in high inversion at the beginning of the transfer from the columns towards the memory. The transfers of the charge-signal and the charge-noise from the memory towards the read-out register or the drain have the same duration and are made by using training charges at least sufficient to allow to pass in high inversion at the beginning of the transfer. These training charges are read with the charge-signal or collected with the charge-noise.

This application is a continuation of application Ser. No. 562,462, filed Dec. 16, 1983 now U.S. Pat. No. 4,611,234.

BACKGROUND OF THE INVENTION

(1) Field of the Invention

The present invention concerns an analysis process of a line transfer photosensitive device. It also concerns an operating device of such a process.

(2) Description of the Prior Art

Photosensitive devices of which the analysis is carried out by line transfer are known in the prior art, especially through U.S. Pat. Nos. 4,430,672 and 4,506,299, each assigned to THOMSON-CSF. However, these devices present drawbacks at the level of efficiency of the charge-signal transfer.

SUMMARY OF THE INVENTION

The present invention thus seeks, with respect to the known solutions that will be set out in the detailed description of the figures, to improve the efficiency of the charge-signal transfer from the conducting columns addressing the photosensitive points up to the read-out register. In fact, the present invention seeks to improve the efficiency of the transfer without degrading certain characteristics of the line transfer photosensitive device, such as;

the noise added to the signal read;

the quantity of charge that must contain the read register.

Indeed, if this charge quantity is important it requires a large size register, thus a high control phase power and important couplings between the control phases;

the vertical resolution at low-level light.

The present invention also seeks to ensure an efficient transfer of charge noise from the columns until the collector or evacuation drain, without disturbing the charge-signal transfer and without using collectors at the level of the photosensitive zone.

The present invention concerns an analysis process of a line transfer photosensitive device, this device comprising a photosensitive zone of M lines of N photosensitive points, the photosensitive points of the different lines being connected in parallel by conducting columns to a memory that ensures the transfer towards a read-out register of the charge-signal of a single line and which ensures the transfer towards a collector of the charge-noise present on the columns prior to the intake of the charge-signal.

According to one characteristic of the invention, the analysis of each line of the photosensitive zone is realized by transferring the charge-signal towards the memory, by superimposing on the charge-signal at least one first training charge sufficient to pass in high inversion at the beginning of the transfer of the columns towards the memory, this first training charge being stored in memory and transferred onto the columns prior to the charge-signal intake, a second training charge, at least sufficient to allow to pass in high inversion at the beginning of the transfer, being superimposed on the charge-signal at the moment of transfer towards the read-out register, this second training charge being read with the charge-signal.

According to another characteristic of the invention, the collection of the charge-noise present on the columns prior to the intake of the charge-signal comprises the following steps:

(1) transfer of the charge-noise of the columns towards the memory by superimposing on it the same first training charge as for the charge-signal, the transfer having the same duration as the transfer of the charge-signal of the columns towards the memory and the first training charge still being stored in memory and periodically transferred onto the columns;

(2) transfer of the charge-noise of the memory towards the collector by superimposing on it a third training charge at least sufficient to allow to pass in high inversion at the beginning of the transfer, this transfer having the same duration as the transfer of the charge-signal transfer of the memory towards the read-out register, and this third training charge being evacuated with the charge-noise towards the collector.

BRIEF DESCRIPTION OF THE DRAWINGS

Other objects, characteristics and results of the invention will appear from the following description given by way of non-limitative example and illustrated by the annexed drawings in which:

FIGS. 1 and 2 are schemes illustrating two analysis processes according to the prior art of a line transfer photosensitive device

FIG. 3 is a curve showing how is carried out in the process of FIG. 2, the transfer of the charge-signal of the intermediate capacitances of the memory towards the read-out register;

FIG. 4 is a scheme illustrating the analysis process according to the invention;

FIGS. 5 and 6 are curves showing how is carried out, in the process according to the invention, the transfers from the column charge towards the intermediary capacitances and from the intermediary capacitances towards the read-out register;

FIG. 7 is a scheme of a device for operating the process according to the invention;

FIGS. 8(a) to (k) are transversal cross-section views of the device of FIG. 7 and schemes explaining its operation;

FIG. 9 is a scheme of a second embodiment of the injection of the third training charge according to the present invention;

FIGS. 10(a) to (k) are transversal cross-section views of the device of FIG. 9 and schemes explaining its operations;

FIG. 11 is a partial scheme of a third embodiment of the injection of the third training charge according to the present invention;

FIGS. 12(a) and 12(b) are transversal cross-section views along A--A of FIG. 11 and a scheme explaining its operation;

FIG. 13 is a scheme of another embodiment of the input stage of the device of FIG. 11;

FIG. 14 is a partial scheme of a fourth embodiment of the injection of the third training charge according to the present invention;

FIG. 15 is a partial scheme of a fifth embodiment of the injection of the third training charge according to the present invention;

FIG. 16 is a time diagram of the phases applied on the register used in FIG. 15.

DESCRIPTION OF THE PREFERRED EMBODIMENT

On the different figures, the same references designate the same elements, but for reasons of clarity, the dimensions and proportions of the various elements have not been respected.

FIG. 1 is a scheme illustrating an analysis process of a line transfer photosensitive device according to the prior art. This process is described in the article published in the periodical I.E.E.E. Journal of Solid State Circuits, volume SC 15, No 2, April 1980, page 206.

FIG. 1 schematically represents a photosensitive zone 1, constituted by a matrix of M lines each comprising N photosensitive points P. This zone receives the luminous image to be analyzed and transforms it into electric charges, called charge-signal. The photosensitive points of a single line are joined to one another and connected to an addressing register 2 that allows to select one line of the matrix. The photosensitive points of one line are connected to a single conducting column.

The charge-signal created in each of the photosensitive points of a single line is transferred in parallel towards a read-out register 3 that supplies the data received in parallel, in series. This data constitutes the video signal of the optical image analysis received on the photosensitive zone 1. The register is preferably of the CCD type charge transfer register.

In the prior art, constituted for example, by the two patents mentioned herein-above, it has been shown that the efficiency of the transfer is improved by superimposing a training charge Q₀ at each charge-signal Q_(S) ; this improvement is above all noticeable when the charge-signal is of low amplitude.

In the article of I.E.E.E. already cited, the training charge is supplied by the read-out register itself. In this case, there is a permanent injection of a quantity of charges Q₀ in the register. The training charge Q₀ is transferred onto each of the columns prior to the intake of the charge-signal on the column, as is symbolised on FIG. 1 by an arrow leading from the register towards each column. Then the whole Q_(S) +Q₀, charge-signal plus the training charge, is transferred from each column to the read-out register and from there in serie to the output. The transfer of Q_(S) +Q₀ of the columns towards the register is symbolized by a double arrow on the figure.

The drawbacks of the analysis process of a transfer line photosensitive device are the following.

Taking into account the relatively large capacity of the columns when the number of lines in high, the training charge Q₀ must be important before the maximum charge-signal. For example, the capacitance of the columns is about 3 pf for 625 ines, which leads to using a training charge Q₀ of about 1 pc for a maximum charge-signal of 0.2 pc. This has undesirable consequences:

at the output of the read-out register, Q_(S) +Q₀ and not simply Q_(S) is obtained. The temporal noise is thus dominated by the noise due to the charge Q₀. It is not possible to inject a high charge into a charge transfer register without superimposing on it a noise bound to the input capacitance of the register and the injection method. The input capacitance of the register, and thus of the associated noise, are as important as the Q₀ is high. The training charge Q₀ being important, one of the advantages of the line transfer, which is to allow low-noise reading, is lost.

Furthermore, it is necessary to contain in the read-out register not Q_(S) but Q_(S) +Q₀. A larger size register is thus necessary, as well as a higher control phase power and more important couplings between the control phases.

Another drawback of the process illustrated by FIG. 1 is that the evacuation of the charge noise due to the "smearing" or the "blooming" can only be realized by drains situated adjacent to the photosensitive points.

The assignee of the present application considers that it is preferable that the reading of the charge noise, like that of the charge-signal, is carried out by using a training charge Q₀.

Then, only a single charge quantity Q₀ is available for each column; since Q₀ is transferred towards the output with the charge-signal, it is not possible to dispose of a training charge Q₀ to read the charge noise. It would thus be necessary to use drains situated at the level of each photosensitive point.

FIG. 2 is a scheme illustrating another analysis process of a line transfer photosensitive device according to the prior art. This process is described in U.S. Pat. No. 4,506,299.

FIG. 2 also shows, with respect to FIG. 1, the presence between the photosensitive zone 1 and the read-out register 3 of a line memory 4. This memory comprises a series of intermediary capacitances C_(i), each capacitance being connected, on the one hand, to a column and, on the other hand, to switchover means symbolized by switches 1 and leading the contents of the intermediary capacitances either towards a drain or towards the read-out register.

According to this process, a training charge quantity Q₀ is stored in each intermediary capacitance. This training charge quantity is transferred onto columns prior to the intake of the charge-signal Q_(S), thereafter the charge quantity Q_(S) +Q₀ is transferred into each intermediary capacitance. These two series of transfers are symbolically represented by arrows on FIG. 2.

It is possible to transfer the charge quantities Q_(S) +Q₀ into the read-out register but it is generally preferable only to transfer thereon the charge quantities which allows the elimination of the noise known as spatial noises existing on Q₀ from one column to another and which allows the read-out register not to be overloaded. The transfer from each intermediary capacitance to the read-out register must thus be carried out in such a way as to leave behind the charge quantity Q₀. This is realized by a potential barrier that only allows to pass the charge-signal Q_(S) in excess with respect to Q₀.

FIG. 3 shows how is carried out over a time t the charge transfer from each intermediary capacitance towards the read-out register. The characteristic Q(t) of FIG. 3 thus shows the discharge in function of time t of the intermediary capacitances. This characteristic comprises a substantially vertical part, an elbow, then a substantially horizontal part.

The transfer is carried out, first of all, in high inversion and, thereafter, in low inversion.

Thus a charge-signal quantity Q_(S1), such as an intermediary capacitance contains a charge quantity Q₀ +Q_(S1) bearing its operating point at the point A of the characteristic Q(t) of FIG. 3, i.e. on the substantially vertical part of this characteristic. After read time t₁, the charge Q_(S1) was transferred into the read-out register. The operating point of the capacitance is at the point B of the characteristic, i.e. in the elbow of the characteristic and this capacitance only contains a charge Q₀₁ hardly different from Q₀. The transfer of Q_(S1) was efficient since it is carried out in high inversion.

The assignee of the present invention has displayed that the process represented in FIG. 3 has the following drawback.

When the charge-signal quantities that are read-out have values substantially equal to Q_(S1), the operating point on the characteristic of FIG. 3 is displaced between two points close to the point A and the point B. The transfer of Q_(S1) is efficient since it is carried out in high inversion.

In fact, the value of the intermediary capacitances being low, this is displayed by a characteristic Q(t) presenting a substantially vertical part. It is therefore sufficient to have a low value charge-signal Q_(S) --of about 0.05 pc, for example--so that the point A is present on the vertical part of the characteristic and that the transfer be efficient and be carried out in high inversion.

On the contrary, the process represented in FIG. 3 performs far less well when it is necessary to process lines that are not, or only barely, illuminated.

In the absence of lighting, the transfer towards the read-out register is carried out, still over a period of time t₁, but from the point B until the point C where the training charge is reduced to the value Q₀₂ so that Q₀₂ <Q₀₁. If several successive lines are without a signal, the operating point will successively pass from C into D . . . then into N. The training charge is little by little reduced and passes from Q₀₁ to Q₀₂ then to Q_(0N). The low inversion transfer that occurs at each reading of the non-illuminated lines ends up by hollowing out a large "pocket" in the training charge Q₀. The next charge signal that will follow the black lines will have to fill in this pocket before it is able to be transferred. The transfer of this charge signal will thus be carried out in low inversion with a greatly reduced transfer efficiency.

Let us suppose, indeed, a charge-signal Q_(S2) that causes the operating point to pass from N to S. The transfer during the time t₁ leads from the point S to the point T.

The charge transferred into the register passing from the point S to the point T is written as:

    Q(t.sub.S)-Q(t.sub.T)=Q.sub.S.sbsb.2 +Q.sub.0N -Q(t.sub.T)

Let us take: Q(t_(T))=Q_(0N) +Q₀, the transfer efficiency will be written as ε=(ΔQo/Q_(S2))

FIG. 3 shows graphically that ε can be higher than 50%.

The process of the prior art represented by FIG. 3 thus produces a considerable loss of the vertical resolution that is much more sensitive as the light level decreases.

Another drawback of the process represented by FIG. 2 is that like the process of FIG. 1, the collection of the charge noise due to the smearing or the blooming can only be realized by drains situated close to the photosensitive dots.

In the process represented on FIG. 2, the training charge Q₀ that is stored in the intermediary capacitances could a priori be used to transfer the charge noise Q_(B) then the charge-signal Q_(S) of the columns into the intermediary capacitances. The conservation of Q₀ in the intermediary capacitances is carried out by using a potential barrier that only allows to pass the charges in excess with respect to Q₀.

The assignee has observed that the conservation of Q₀ in the intermediary capacitances during the charge-signal transfers and the charge noise of the intermediary capacitances towards the read-out register raise the two following problems:

two potential barriers are necessary to retain Q_(O) in the intermediary capacitances, whereas the charges are transferred either towards the drain or towards the read-out register. It is practically impossible to obtain the strict egality of these two barriers. The solution to this problem consists in using a double stage line memory such as that described in U.S. Pat. No. 4,506,299 and which is represented on FIGS. 8 and 9 of that application;

FIG. 3 and its commentary have shown the problems that are raised during the charge-signal transfer of the intermediary capacitances towards the read-out register, by retaining Q₀ in the intermediary capacitances and this when the lines that are not, or only barely, illuminated are processed. When the charge noise is transferred from the intermediary capacitances towards the read-out register, Q₀ being retained in the intermediary capacitances, the following problem thus occurs. It has been seen that in the absence of lighting, the transfer is always carried out towards the read-out register, during a time t₁ and that the training charge is thus reduced. The intake of the charge noise does not necessarily allow to pass again into high inversion, but allows to give back to the training charge a value more or less close to Q₀ according to the quantity of charge noise that is transferred. If the next quantity of charge-signal to be transferred is substantially null a charge quantity is, even so, read that is practically proportional to the charge noise previously read out and that has more or less restored Q₀. There is thus a very poor efficiency for the collection of the charge noise.

FIG. 4 is a scheme illustrating the analysis process of a line transfer photosensitive device according to the invention.

As in the process represented in FIG. 2, a training charge quantity Q₀ is stored in the memory in each intermediary capacitance and transferred onto the columns prior to the intake of the charge-signal Q_(S). Thereafter, the charge quantity Q₀ +Q_(S) is transferred into each intermediary capacitance, and likewise for each reading.

FIG. 5 shows how is carried out in time the transfer of the charges from the columns to the intermediary capacitances. This characteristic Q(t) presents an elbow much more pronounced than the characteristic of FIG. 3 since the capacity of the columns is much more important--about ten times more important--than that of the intermediary capacitances.

Let us suppose that there was no charge-signal to be transferred from the columns towards the memory, the operating point is situated at the point A of the curve represented in FIG. 5. The charge to be transferred equals: Q₀ +Q_(r), with Q₀ the training charge stored in the intermediary capacitances and Q_(r) a residual charge.

After a reading time T_(L), the operating point passes from the point B. The charge Q₀ was transferred into an intermediary capacitance. The charge of the column is only Q_(r). The return of Q₀ on the column prior to a new reading of the charge-signal brings the operating point back to point A. In the absence of any charge-signal to be transferred, the charge of the columns moves at each reading between the two balancing positions that are the point A, where the charge is equal to Q₀ +Q_(r) and the point B, where the charge is equal to Q_(r).

When non null charge-signal Q_(S) is transferred from the photosensitive zone onto a column, the operating point passes into S where the charge equals: Q₀ +Q_(r) +Q_(S).

After reading time t_(L), the operating point passes into a point B' very close to B, where the charge equals Q'_(r). The point B' is very close to the point B since the inclination of the characteristic Q.sub.(t) is very high at the point A and low at the point B.

The fact that the point B' is distinct from the point B signifies that a quantity of charge ΔQ_(r) has not been transferred.

The charge transferred on one intermediary capacitance when the operating point passes from S into B is written as follows: charge in S charge in B' ##EQU1## with ΔQ_(r) =Q'_(r) -Q_(r). Then, ΔQ_(r) can also be expressed in function of Q'(t_(B)), which is the inclination of the characteristic at the point B:

    ΔQ.sub.r =Δt.Q'(t.sub.B)                       (1)

where, Δt is the projection of the segment BB' on the axis of times.

The projection of the segment SA on the axis of times also equals Δt, from which the following relation causing to intervene Δt:

    Q.sub.S =Δt.Q'(t.sub.A)                              (2)

where, Q'(t_(A)) is the inclination of the characteristic at the point A.

The efficiency of the transfer is thus expressed by using relations (1) and (2) in function of the ratio of the characteristics to the points B and A: ##EQU2##

In order to obtain a good transfer efficiency, it is necessary that the point A be in a steep inclination zone, thus of high inversion, and that the point B be in a weak inclination zone, thus of low inversion.

According to the invention, the minimum amplitude of the training charge Q₀ must be such that it allows to pass in high inversion at the beginning of the transfer of the columns towards the memory, even if there is no charge signal to be transferred. This is the condition to have a good transfer efficiency of the charge of the columns towards the line memory.

This charge quantity Q₀ is that much greater as the capacitance of the columns is higher.

Indeed, the inclination of the left-hand part of the curve shown on FIG. 5 that corresponds to an operation in high inversion decreases as the square of the capacitance of the columns. Furthermore, for a given technology, the capacitance of the columns increases with the number of lines to be analysed.

This thus explains the necessity of an important training charge Q₀ before the maximum value of the charge signal if it is desired to obtain a good transfer efficiency at the reading of a photosensitive device comprising a high number of lines, 625 lines, for example.

For example, for C columns ≃3.5 pf, it is necessary to select a training charge of about 1 pc, while Q_(S) is about 0.2 pc, for a reading time T_(L) of about 2 μs. A transfer efficiency of about 3% is thus obtained.

According to the invention, the charge-signal transfer of the memory in the read-out register is carried out by superimposing on the charge-signal a training charge Q₁. This charge Q₁ must be chosen so as to allow to pass in high inversion at the beginning of each transfer of the charges, from the memory towards the register, even when there is no charge-signal to be transferred and by taking into account the fact that Q₁ is superimposed on Q_(O) stored in the memory. Thus the loss of vertical resolution is prevented which occured in the process represented in FIG. 2 when there is no charge-signal to be transferred.

FIG. 6 represents the characteristic Q(t) for the transfer of the memory in the read-out register. The training charge Q₁ allows to pass from the point B (where the charge equals Q₀) to the point A (where the charge equals Q₀ +Q₁) or to the point A' (where the charge-equals Q₀ +Q₁ +Q_(S)) when there is a charge-signal to be transferred. The points A and A' are situated in a zone of high inversion.

Thus after reading time t₁, the operating point is again substantially in B without dropping below in the absence of the signal.

The training charge Q₁ must be supplied at each reading since it is read with the charge-signal.

The training charge Q₁ can be supplied in different ways.

These charges can be supplied by the read-out register. In this case, there is permanent injection of a charge quantity Q₁ in the register. A training charge Q₁ is thus transferred on each intermediary capacitance before the intake of the charge-signal. Thus supplied, the charge quantities Q₁ are identical and do not introduce any supplementary spatial noise.

The training charges Q₁ can also be injected on each intermediary capacitance from a diode associated to an injection gate. In this case, there is fear of introducing a spacial noise on the charges quantities Q₁.

It is also possible to inject training charges Q₁ directly at the level of the photosensitive zone by using the technique of shower lighting. In this case a uniform lighting is available that permanently generates in the photosensitive points a charge Q₁ that is superimposed on the charge-signal and the training charge Q₁ will be read with the charge-signal Q_(S). As the charge amplitude Q₁ is low, the quantum noise associated to its generation is of little importance. On the other hand, the presence of this constant charge in each photosensitive point presents the advantage of improving the transfer of the photosensitive point towards the column and of suppressing the remanence in the case where the photosensitive point is constituted by a photodiode and a photo-MOS.

In the case of a device covered by colored filters, it is essential that the lighting be chosen so as to be transmitted in a uniform manner by the different filters. A lighting in the near infrared, for example, can be used, for which the colored filters all have in general an equivalent transmission.

The intermediary capacitances having a relatively low value, it is sufficient to use a relatively low charge Q₁ in order to come back in high inversion at each reading from, for example, the point B of the characteristic Q(t) of FIG. 6. Typically, the training charge Q₁ may be about Q_(S) max/10, where Q_(S) max represents the highest value of the charge-signal. It is preferable to select the minimum training charge Q₁ that allows to come back in high inversion at each reading from point B. Thus the temporal injection noise associated to Q₁ is clearly lower than that associated to the charge Q_(O) transferred in the read-out register in the case of the process of FIG. 1. Neither is there the drawback of the process of FIG. 1 with respect to the total charge quantity that must contain the read-out register since the driving charge Q₁ only increases by about 1/10th the dynamic of the signal to be transported in the read-out register.

The charge noise Q_(B) introduced on the columns by smearing or overlighting must be evacuated towards the drain before the intake of the charge-signal.

The assignee considers it is preferable that the transfer of the charge noise Q_(B) like that of the charge-signal is carried out with a double training charge.

As concerns the transfer of the columns towards the memory, the same training charge Q₀, that is stored in the memory is used to transfer the charge-signal and charge-noise. Thus, the equilibrium potential of the columns, i.e. the point B of the characteristics of FIGS. 5 and 6, is not disturbed. Furthermore, it is necessary that the transfer time T_(L) is the same for the charge-signal and the charge noise.

With respect to the transfer of charges of the memory towards the drain or towards the read-out register, a training charge Q₁ is used to transfer the charge-signal Q_(S) and a training charge Q₂ to transfer the charge noise Q_(B).

When the transfer of the memory towards the drain or towards the read-out register is achieved, there is a substantial return to the point B of the characteristic of FIG. 6 where the charge is equal to Q₀.

It has been seen that the charge Q₁ was selected to allow to pass in high inversion at the beginning of each charge transfer from the memory towards the register, even when there is no charge-signal to be transferred. The intake of Q₁ on an intermediary capacitance C₁ brings the operating point to the point A. The transfer of Q_(S) +Q₁ during the time t₁ brings back the operating point close to the point B.

The training charge Q₂ is selected, like Q₁, in order to allow to pass in high inversion at the beginning of each charge transfer, even if there is no charge noise to be transferred.

The intake of Q₂ brings the operating point of the point C then the intake of Q_(B) brings it to the point C'. The transfer of Q_(B) +Q₂ during the same time t₁ as that which is used to transfer Q_(S) +Q₁ brings the operating point close to the point B. On the other hand, the charge Q₂ being evacuated, it is not particularly worthwhile to select, as for Q₁, the minimum charge allowing to come back in high inversion at each reading of the point B.

The operating point obtained following the transfer of the charge-signal and the charge noise of the memory towards the drain or the register is not strictly the point B since the quantities Q_(S) +Q₁ and Q_(B) +Q₂ are not necessarily the same and since the inclination of Q(t) at the points A' and C' is not infinitive. However, the intermediary capacitances having fairly low values, the inclinations at points A' and C' and the ratios Q'(t_(A))/Q'(t_(B)) and Q'(t_(C))/Q'(t_(B)), are high and are thus brought back close to the point B, thus with a charge on the columns that is close to Q₀.

From what is set out herein-above, it means that it would be preferable that the training charges Q₁ and Q₂ be equal, but it is not absolutely obligatory. This depends on the quantity of spatial noise tolerated at the output of the device.

The charges Q₂ being evacuated in the drain, while the charges Q₁ are read with the signal, the charges Q₂ can be introduced in any possible manner, from the moment that their amplitude is sufficient to pass again in high inversion at each transfer from the point B.

The training charge Q₂ can be introduced into the memory from the evacuation drain. However, such an introduction method of the charges generally results in a dispersion on the value of the third training charge from column to column of about 20%. On the other hand, the inefficiency of transfer between the intermediary capacitances of the line memory is not null Is thus restored, superimposed on the charge-signal, a residual charge issuing from the third training charge including of any eventual spatial noise bound to the introduction of this third training charge.

Consequently, as explained herein-above, other methods can be used to introduce the training charge Q₂.

FIG. 7 is a scheme of a device for operating the process according to the invention using the evacuation drain for the introduction of the training charge Q₂.

The top of FIG. 7 represents a photosensitive zone 1. The photosensitive points are disposed in a matrix. A gate G separates each photosensitive point of the column connections. This gate allows to isolate the photosensitive points from the rest of the device during the integration of the charges.

The conducting columns lead to a double stage line memory such as that described in U.S. Pat. No. 4,506,299 and which is represented in FIGS. 8 and 9 of this application.

This memory comprises a series of intermediary capacitances C₁ in which are stored the training charges Q₀. A gate G_(P) controls the passage between each column and an intermediary capacitance. The potential of this gate fixes that of the columns.

These intermediary capacitances are followed by switchover means that lead the contents of the intermediary capacitances either towards an evacuation drain or towards a read-out register.

FIG. 7 shows that the intermediary capacitances C₁ are followed by gate G₀ allowing to retain the driving charges Q₀ in the intermediary capacitances and that fix their amplitude. The gates G₀ are followed by capacitances C₂ that act as dispatchers and allow to send charges coming from C₁ either towards the evacuation drain after passage of a gate R, or towards the read-out register 3, after passage of a gate C. The access to each capacitance C₂ is controlled by three gates, a gate G₀ that allows the intake of the charges and two gates R and C that allows their departure either towards the drain or towards the read-out register.

This double stage line memory allows to retain the training charge Q₀ by an independant potential barrier of the dispatching elements either towards the drain, or towards the read-out register.

FIG. 8 is a transveral cross-section view of the device represented in FIG. 7. It is followed by schemes showing the evolution of the surface potential φ_(S) in the semi-conductor substrate 5 on which the photosensitive device is integrated, at various instants, taken during one read line sequence made according to the process of the invention. The hatched zones indicate the presence of minority carriers. FIGS. 8b to k only represents the interface 6 of the substrate and the insulating layer that covers it.

FIG. 8b shows the photosensitive points that are integrated from the charges and contain a quantity of charge-signals Q_(S). On the columns, can be seen the training charge Q₀ and charge noise Q_(B). The drain imposes a certain level of charges in the capacitances C₂.

FIG. 8c shows the training charge Q₂ isolated under the capacitances C₂ by the return of the gate R to the low level.

FIG. 8d shows the transfer of the columns towards the intermediary capacitances of the charge noise Q_(B) and the training charge Q₀ due to the increase of the potential of the gate G_(P). This transfer is carried out during time T_(L). Simultaneously, the capacitances C₂ pass to the low level and the training charges Q₂ are transferred onto the intermediary capacitances C₁.

FIG. 8e shows the transfer of Q_(B) +Q₂ of C₁ towards C₂ then towards the drain during time t₁. The capacitance C₂ and the gate R are thus at the high level. The training charge Q₀ is retained under C₁ by G₀.

FIG. 8f shows C₁ and C₂ passing at the low level. The charge Q₀ returns onto the columns and the charge Q_(B) +Q₂ is completely evacuated towards the collector.

On FIG. 8g, C₁ and C₂ return to the high level.

On FIG. 8h, there is a transfer of the charge-signal Q_(S) of the photosensitive points on the columns where they are added to the charges Q₀. Simultaneously, there is a transfer of training charges Q₁ in the capacitances C₂. These charges issue from the read-out register where they are injected permanently during the previous line time.

It is the passage at the high level of the gate C that allows their transfer into C₂.

On FIG. 8i, the passage of the gate G_(P) at the high level allows the passage of Q₀ +Q_(S) in C₁ during a time T_(L).

Furthermore, the passage of C₂ at the low level provokes the transfer of Q₁ under C₁.

On FIG. 8j, the passage of C₂ and the gate C at the high level allows the passage of Q_(S) +Q₁ of C₁ towards C₂ during the time t₁ then towards the register. The charge Q₀ is retained under C₁ by the gate G₀.

On FIG. 8k, the passage of C₁ and C₂ at the low level provokes the return of Q₀ on the columns and the complete transfer of Q_(S) +Q₁ in the register.

On the columns, to the charge Q₀ is added to charge noise Q_(B) and there is a return to the situation of FIG. 8b.

The stages represented on FIGS. 8b to k occur, preferably, during the line return time.

With the device represented on FIG. 7, it is possible to use a process other than that described herein-above to generate the second and third training charges Q₁ and Q₂.

Thus, the second training charge Q₁ can be obtained by using the shower lighting technique, the third training charge Q₂ being obtained by injecting continuously the said charge into read-out register 3. In this case, the second training charge Q₁ is generated permanently due to a uniform lighting at the level of the photosensitive points they are superimposed on the charge-signal. This second training charge is thus read with the charge-signal Q_(S). With respect to operating, it is identical to that described with reference to FIG. 8 when it involves the transfer of charges Q_(B) +Q₂ or Q_(S) +Q₀ +Q₁ but it differs slightly in the processes used to superimpose the third training charge Q₂ on the charge noise Q_(S). Indeed, in this case, the second training charge Q₁ is superimposed on the charge signal Q_(S) at the level of the photosensitive point and it is the whole of total Q_(S) +Q₁ that is transferred from the photosensitive point on the corresponding column where it is added to the charge Q₀.

Furthermore, the third charge Q₂ is transferred from the read-out register 3 towards the capacitance C₂, the gate R being at the low level and the gate C being at the high level instead of being imposed by the level in the drain.

FIG. 9 is a scheme of another embodiment of a device operating the process of the present invention using a CCD register for the injection of the third training charge Q₂.

On this figure, the photosensitive zone 1, the line memory 4 and the read-out register 3 are identical to those of FIG. 7. Consequently, they will not be described again in detail.

However, according to the a represented embodiment, a shift CCD type register 10 having serie input and parallel outputs is positioned in parallel to the lines of the photosensitive matrix on the side opposite to the read-out register 3. This register 10 is separated from the photosensitive matrix by gates C' that regulate the moment of the transfer of the charges Q₂ towards the columns of the photosensitive matrix. The third training charge Q₂ is injected continuously in a shift register 10 by the intermediary of a known injection type state constituted by a diode and gates.

The operation of this embodiment will be explained with reference to FIGS. 10(a) to 10(k). FIG. 10(a) is a transversal cross-section view of the device of FIG. 9. This figure represents in a broken line a storage stage of the shift register 10 and a storage of the read-out register 3, these stages being referenced, respectively, by φ_(CD) and φ_(CCD).

FIGS. 10(b) to 10(k) are schemes showing the evolution of the surface potential φ_(S) in the semi-conductor substrate 5 on which is integrated the photosensitive device, at various instants taken during a line reading sequence made according to the process of the invention. The hatched zones indicate the presence of minority carriers: FIGS. 10(b) to 10(K) represent simply the interface 6 of the substrate and of the insulating layer that covers it.

According to the present invention, during the line time at which is carried out the serie output of the video signal in the read-out register 3, the second and third training charges Q₁ and Q₂ are injected in serie in the charge transfer registers 3 and 10 so that at the end of the line time Q₁ and Q₂ are present on the parallel outputs of the registers herein-above.

Due to this fact, at the beginning of line return time, the state of operation is that represented in FIG. 10(b). On this figure, Q_(S) represents the integrated charge signal at the level of each photosensitive point. Furthermore, the first training charge Q_(O) and the charge noise Q_(B) are positioned on the columns and the charges Q₂ and Q₁ are present in the corresponding stages of the shift registers 10 and 3.

As shown in FIG. 10(c), the charge Q₂ is transferred from the shift register 10 towards the columns where is present the principal training charge Q₀. To do this, the gate C' is positioned at a high level and the potential φ_(CCD) is positioned at a low level.

Thereafter, as represented in FIG. 10(d) the whole of the charges Q₀ representing the first training charge, Q₂ representing the third training charge and Q_(B) representing the charge noise such as the blooming charges, for example, is transferred on the columns towards the intermediary capacitance C₁ due to the increase of the potential of the gate G_(P). Simultaneously, the capacitances C₂ pass to the low level and the training charges Q₂ as well as the charge noise Q_(B) are transferred towards the capacitance C₂ then towards the drain DR, the potential of the gate R being present at a high level, whereas the charge Q₀ is maintained in the capacitance C₁ by the potential barrier created under the gate G₀, as represented on FIG. 10(e).

As represented on FIG. 10(f), the capacitances C₁ and C₂ pass at the low level. Due to this fact, the charge Q₀ returns on the columns and the charge Q_(B) +Q₂ is completely evacuated towards the drain DR.

On FIG. 10(g), the capacitances C₁ and C₂ return to the high level and the potential of the gate R is brought back to the low level.

Thereafter, as represented in FIG. 10(h), there is a transfer of charges Q_(S) from the photosensitive points to the columns where they are added to the first training charges Q₀. Simultaneously, the second training charges Q₁ stored in the storage stages of the read-out register 3 are transferred in the capacitances C₂ during the passage at the high level of the gate C.

Then, as represented on FIG. 10(i), the passage of the gate G_(P) at the high level allows the passage of the charges Q₀ +Q_(S) in the intermediary capacitances C₁.

Furthermore, the passage of the capacitance C₂ at the low level provokes the transfer of the second training charge Q₁ under the intermediary capacitances C₁.

As represented on FIG. 10(j), the passage of the capacitances C₂ and of the gate C at the high level allows the passage of the charges Q_(S) +Q₁ of the capacitance C₁ towards the capacity C₂ then towards the read-out register 3. The charge Q₀ is retained under the intermediary capacities C₁ by the gate G₀.

On FIG. 10(k) the passage of the capacitances C₁ and C₂ at the low level provoke the return of the first training charge Q₀ on the columns and the transfer of Q_(S) +Q₁ in the read-out register according to the process described with reference to FIG. 8.

On the columns, to the charge Q₀ is added the charge noise Q_(B) and there is a return to the situation of FIG. 10(b).

The stages represented on FIGS. 10(b) to 10(k) took place preferably during the line return time.

The second and third training charges Q₁ and Q₂ being injected in series in the CCD type shift register, they are, due to this fact, free from spatial noise, which could not be realized when the third training charge Q₂ was obtained by using a drain.

FIGS. 11 to 13 represent another embodiment according to the present invention of the injection device of the second and third training charges. This injection device is more particularly interesting in the case where the transfer line photosensitive device comprises two read-out register line memory assemblies situated one above and the other underneath the photosensitive matrix, allowing to read alternately the odd and even columns of this matrix, as described, for example, in French patent application No. 81 06432 in the name of the assignee. However, it is evident for the man skilled in the art that this device can also be used in the case of a single read-out register line memory assembly as described with reference to FIGS. 9 and 10.

As represented in FIG. 11, in which, for simplicity's sake, has been omitted the photosensitive matrix 1 and solely referenced by 4 the line memory, the injection devices of the second and third training charges Q₁ and Q₂ are respectively constituted by the read-out register 3 and by an auxiliary charge transfer register 11 positioned parallel to the read-out register 3 and beside it. The two registers 3 and 11 are controlled by common phases φ₁ and φ₂ and communicate at the level of each phase φ₁, by the intermediary of a gate of passage φ_(P).

Insulating diffusions 12 are provided between the two registers 3 and 11 at the level of phases φ₂.

Furthermore, as represented in a more detailed manner on FIG. 12(a) that is a transversal cut along A--A of FIG. 11, the read-out register is of the volume transfer type while the auxiliary register 11 is of the surface transfer type. This allows to have lower potentials in the auxiliary register than in the read-out register for a same applied voltage φ₁ and consequently allows the transfer of the charges stored in the auxiliary register towards the read-out register by bearing simply the potential of the gate φ_(P) at the high level, as will be explained in further detail herein-after. Furthermore, to clearly separate the two transfer channels of the charges of the registers 3 and 11, an insulating diffusion 16 is provided under the gate φ_(P).

As represented on FIG. 11, the second and third training charges Q₁ and Q₂ are obtained by injecting a single charge Q_(e) in the input stage and by sharing this charge Q_(e) into two equal parts Q₁ and Q₂ by using an insulating diffusion 13 according to the process described in French patent application No. 77 28737 in the name of the assignee.

As represented on FIG. 13, the charges Q₁ and Q₂ can be obtained from two independant injection stages 14, 15 one for Q₁ and the other for Q₂.

The operation of this embodiment will now be explained with particular reference to FIGS. 11 and 12.

During the line time, the charges Q₁ and Q₂ are injected in series on each stage of the two adjacent registers 3 and 11. The training charge Q₂ being, first of all, used for the evacuation of charge noise, it will be injected in the read-out register 3 while the second training charge Q₁ will be injected in the auxiliary register.

At the beginning of line return time, the third training charge Q₂ injected in the read-out register 3, is transferred in the line memory 4 by positioning gate C at a low level, to be used as a charge noise training charge Q_(B). The charge Q₂ is thus injected in the capacitance C₂ and its use as a third training charge is realized in the same way as when the charge Q₂ is obtained in the capacitance C₂ from the drain as described with reference to the FIGS. 8(a) to 8(K).

Once the whole of the charges Q₂ +Q_(B) evacuated in the drain DR, the training charge Q₁ is transferred from auxiliary register 11 towards the corresponding stage of the read-out register 3 by carrying the potential barrier under φ_(P) to a high level as represented on FIG. 12(b). Thereafter, the barrier under φ_(P) being brought back to the low level, the charge Q₁ is transferred from the read-out register 3 towards the line memory to be used as training charge of the charge signal as explained in a detailed manner with reference to FIGS. 10(h) to 10(k). The whole of the charges Q₁ +Q_(S) is thus transferred in the read-out register 3 to be sent towards the output during the following line time simultaneously with new training charges Q₁ and Q₂ being injected in registers 3 and 11.

In the embodiment of FIGS. 11 to 13 is described a surface transfer type auxiliary register. However, the auxiliary register 11 can also be of the volume transfer type, but in this case the quantity of impurities for part N must be smaller than that of the read-out register, so as to obtain an arrangement of potentials in the registers 3 and 11 such as that represented in FIG. 12(b).

FIG. 14 schematically represents an embodiment allowing the injection of the third training charge Q₂ with the use of a shift register.

According to the embodiment represented, the second and third training charges Q₁ and Q₂ are injected directly into a single charge transfer register, namely in the read-out register. However, the read-out register comprises a number of stages that allows to successively store the second and third charge quantities used for a line memory stage.

As represented on FIG. 14, in the case of a bi-phased operating charge transfer register, the register comprises a number of stages which is twice the number of columns. Due to this fact, the charge transfer register comprises four storing electrodes for a line memory stage. In this case, the second and third training charges Q₁ and Q₂ are strictly identical since they are injected in a single charge transfer register.

The operating of the device described herein-below will now be described.

During the line time, the charges Q giving the charges Q₁ or the charges Q₂ according to their position are injected on the whole shift register. Thereafter, the charge Q₂, namely the charge Q present under the storage electrode positioned opposite the gate C, is transferred in the line memory for the evacuation of the charge noise by bringing the potential of the gate C to a high level. It is obvious that the gates C are only provided between the storage electrode of the register 3 opposite the capacity C₂, while the insulating diffusions are provided between the other storage electrodes of the register 3 and the line memory 4.

Once the evacuation of the charge noise towards the drain is realized, the charge Q₁ is transferred twice in the read-out register so as to be present under the storage electrode in communication with the line memory. The charge Q₁ is thus transferred in the line memory to carry out the reading of the charge signal and transfer the whole of the charges Q₁ +Q_(S) in read-out register 3, as described herein-above with reference to FIG. 8 or FIG. 10.

With bi-phase charge transfer registers, it is necessary to double the number of stages of the register to realize the injection of Q₁ and Q₂ in the same register. However, it is obvious for the man skilled in the art, that shift registers with a different number of control phases can be used. In this case, the number of stages of the read-out register does not necessarily have to be doubled. Thus, a three-phase control read-out register can be used that will only comprise three transfers for one line memory stage and that will allow to inject simultaneously the second and third charges Q₁ and Q₂ in a single read-out register.

FIG. 15 again represents another embodiment of a device allowing the injection of the second and third training charges Q₁ and Q₂ through the intermediary of a shift register.

As represented on FIG. 15, the shift register used for the injection of Q₁ and Q₂ is a register of which the storage electrodes that are not in communication with the line memory are separated in two. Each part of the electrode 17, 17' is connected respectively to a phase φ₁ or φ'₁. The cut-off of the electrode is preferably situated in the middle of the transfer channel and is associated to an insulating diffusion 18 that thus realizes a sharing of the charge Q into two equal parts Q₁ =Q₂ =Q/2. It is not necessary that the separation of the charge Q is made along two identical charges Q₁ =Q₂ =Q/2 from the moment that the charges Q₁ or the charges Q₂ remain identical with a sufficient value of the level at each stage of the line memory. The electrodes 19 in communication with the line memory 4 are controlled by a phase φ₂ and are not shared.

An explanation will now be given with particular reference to FIG. 16 that represents the potential applied on the different phases φ₁, φ₁, φ₂ in function of time, the operation of the single register 3 described herein-above.

During the line time a charge Q is injected in series on each stage of the register. The control phases φ₁ and φ'₁ are thus constituted by identical voltages in tooths and phase φ₂ is constituted by a identical voltage in tooths but in phase opposition with phases φ₁ and φ'₁ so as to realize the shift of the charge Q in all the stages of the register. The transfer is interrupted at the beginning of the line return time so that the charge Q is found under the electrodes 17, 17'. This charge Q is thus shared in the form Q₁ =Q₂ =Q/2 under each part of the electrodes 17, 17'.

At the time t₁, the phase φ'₁ is brought to the low level which transfers the charge Q₂ under the electrode 19, the phase φ₂ being carried to the high level. Thereafter, at the time t₂ the phase φ₂ passes to the low level and the gate C of the line memory is simultaneously positioned at the high level. The charge Q₂ is thus transferred in the line memory for the evacuation of the charge noise towards the drain.

During this operation, the phase φ₁ passes simultaneously to the low level to prevent the charge Q₂ from flowing under the electrode 17 to the right of electrode 19.

At time T₃ the phase φ₂ is thus brought to the high level.

At this moment, the charge Q₁ which is present under the electrode 17 is transferred under the electrode 19, then at time T₄ the phase φ₂ returns to the low level and transfers the charge Q₁ in the line memory to carry out the reading of the charge-signal in a manner known per se. The whole of the charges Q₁ +Q_(S) is thus reinjected in the charge transfer device 3 also used as read-out register, so as to realize the reading in series of the charge signal.

Furthermore, in the case where the shift registers used for the injection of the second and third training charges do not present sufficient transfer efficiency, it is possible to overcome this drawback by using registers presenting a number of stages slightly superior to the number of stages of the line memory and by thus eliminating the first charges injected in the shift register. 

We claim:
 1. A line transfer photosensitive device comprising a photosensitive zone of M lines of N photosensitive points, the photosensitive points of the different lines being connected in parallel by conducting columns to a memory that ensures the transfer towards a read-out register of the charge-signal (QS) of a single line and which ensures the transfer towards a drain of the charge-noise (QB) present on the columns prior to the intake of the charge-signal, wherein the line memory (4) comprises a series of intermediary capacitances (C1), each capacitance being connected on either side of the columns to switchover means leading the contents of the intermediary capacitances either towards the drain or towards the read-out register.
 2. Device according to claim 1, wherein the line memory (4) is a double stage memory of which the switchover means comprise a series of capacitances (C2), the access to each capacitance (C2) being controlled by three gates, namely a gate (G0) between the corresponding intermediary capacitances (C1) and capacitance (C2), a gate (R) between the drain and capacity (C2) and a gate (C) between the read-out register (3) and capacitance. 